EP0203765B1

EP0203765B1 - Colour cathode ray tube device

Info

Publication number: EP0203765B1
Application number: EP86303792A
Authority: EP
Inventors: Taketoshi Toshiba Corp. Principal Office Shimoma; Kumio Toshiba Corp. Principal Office Fukuda
Original assignee: Toshiba Corp
Current assignee: Toshiba Corp
Priority date: 1985-05-21
Filing date: 1986-05-19
Publication date: 1990-01-10
Anticipated expiration: 2006-05-19
Also published as: KR890004872B1; EP0203765A3; US4820958A; KR860009466A; DE3668258D1; EP0203765A2

Description

This invention relates to a colour cathode ray tube device with an in-line electron beam arrangement.
The envelope of a colour cathode ray tube consists of a neck in which are installed three electron guns that generate three electron beams which are aligned in the horizontal direction; a face plate having a phosphor screen on its inside face; and a funnel disposed between the neck and the face plate. ^I
The electron beams emitted from the in-line type electron guns are directed on to the phosphor screen, which is formed of coated phosphor layers, causing the phosphor layers to emit light. In order to achieve good colour reproduction with the light emitted from the phosphor layers, the electron beams must be made to impinge selectively on prescribed phosphor layers. This is achieved by positioning a shadow mask formed with a large number of apertures within the envelope close to the face plate.
The in-line electron guns incorporate separate cathodes and are designed so as to generate three electron beams in a common horizontal plane and bring them to convergence in the vicinity of the face plate.
To make the phosphor screen of a colour cathode ray tube display a TV picture, the electron beams must be scanned over the entire surface of the phosphor screen. This is done by mounting a deflection device outside the cone portion of the funnel. Essentially the deflection device comprises deflection coils for generating a magnetic field that deflects the electron beams in the horizontal direction and deflection coils for generating a magnetic field that deflects the electron beams in the vertical direction. In practical colour cathode ray tubes, because of the leakage field that extends beyond the edges of the coils, convergence of the three electron beam spots on the face plate is lost. Various countermeasures have to be adopted to deal with this, so that the spots always converge over the whole surface of the screen.
As explained above, the quality of colour cathode ray tubes has been improved by many technical developments. However, as large tubes have become common, fresh problems have come to the fore.
One of these problems concerns the shape of the beam spot where the electron beams are brought to convergence on the face plate after being shot out from the electron guns. As shown in Figure 1 a of the accompanying drawings, in the middle of the screen where the beams are not subjected to any deflection, the spot S1 a consists simply of a round core Sc, i.e. a region of high electron density. However, as shown in Figure 1b, due to non-uniformity of the deflection magnetic field, in the peripheral regions of the screen, where the spot S1b is subject to deflection the spot presents a fJattened core Sc with vertically extending flares Sf, i.e. portions of lower electron density. As a result, the electron beam size increases at the edges of the screen producing a deterioration in focusing property and resolution.
Specifically, if we take the horizontal dimension of the core for the case of a 20 inch 90 degree deflection tube as CH and its vertical dimension as CV, in the middle of the screen CH=CV=1.0 mm, but, at the extreme end region of the horizontal deflection, the core has a very flattened shape with CH=2.0 mm and CV=0.3 mm. Also, the dimension FV from the top to the bottom of the flares is 1.5 mm. These values are for the case where the electron beam is deflected in the horizontal direction only. In the corners of the screen, where a vertical deflection is added to the horizontal deflection, the dimensions are even more distorted.
French-A-2186794 discloses a colour cathode ray tube of the type to which the present invention relates and where means are provided for applying a time delay to the time at which the picture signals of the respective colours red, green and blue input to the electron guns are controlled, said time delay corresonding to the off-set and the speed of the beam spots on the screen.
It is an object of this invention to provide a colour cathode ray tube device which overcomes the above-mentioned drawbacks, wherein high resolution is obtained over the whole area of the screen with little distortion of the electron beam spot at the peripheral parts of the screen.
According to this invention, a colour cathode ray tube device comprises an envelope having a face plate, a funnel and a neck; a phosphor screen formed on the inside of said face plate and which emits light in the three colours, red, green and blue; in-line electron guns arranged in the neck to generate and direct three electron beams towards the screen, the beams being in-line and mutually parallel in the horizontal direction of said phosphor screen; a shadow mask arranged in the vicinity of said phosphor screen and having a large number of apertures to make said electron beams selectively impinge on said screen; and a deflection device attached outside said funnel and comprising a first magnetic field generating device that generates a substantially uniform horizontal deflection magnetic field that deflects said electron beams in the horizontal direction; a second magnetic field generating device that generates a barrel-shaped vertical deflection magnetic field that deflects said beams in the vertical direction; and means for applying a time delay to the time at which the picture signals of the respective colours red, green and blue input to said electron guns are controlled; characterised in that the half-width, on the tube axis, of the magnetic flux density distribution of said horizontal deflection magnetic field is in the range from 0.1 to 0.4 times the distance from the centre of said flux density distribution to said phosphor screen.
. In order that the invention may be more readily understood, it will now be described, by way of example only, with reference to the accompanying drawings, in which:-

Figures 1a and 1b are views explaining the shape of the electron beam spot in prior art devices;
Figure 2 is a cross-sectional view of an embodiment of this invention;
Figures 3a and 3b are cross-sectional views along the line III-III of Figure 2, Figure 3a being given in explanation of the horizontal deflection magnetic field and Figure 3b being given in explanation of the vertical deflection magnetic field;
Figure 4 is a sketch explaining the magnetic flux density distribution on the tube axis Z of the horizontal deflection magnetic field according to this invention;
Figures 5, 7 and 8 are views explaining the shape of the electron beam spot according to this invention;
Figure 6 is a graph explaining the relationship between the deflection magnetic field according to this invention and the shape of the electron beam spot; and
Figure 9 is a cross-sectional view of another embodiment of the invention.

Noting that one of the factors producing distortion of the electron beam spot at the periphery of the screen is the pin-cushion shape of the horizontal deflection magnetic field, the inventors tried making the horizontal deflection magnetic field uniform, while the vertical deflection magnetic field remained barrel-shaped. Figure 5 shows the electron beam spot shapes S5a and S5b at the centres of the screen and at the periphery of the screen, respectively, for a uniform horizontal deflection magnetic field H, as shown in Figures 3a and 3b. In a 20 inch 90 degree deflection tube, CH=1.5 mm and CV=0.6 mm, and it can be seen that the shape of the region of high electron density, i.e. the core Sc, is much improved.
However, the shape of this electron beam spot is still not fully satisfactory.
By further experiments, it has been found that, if a prescribed relationship between the magnetic flux density distribution of the deflection magnetic field and the size of the colour cathode ray tube is established, the shape of the flares Sf around the core Sc can be further improved.
Figure 4 shows the relationship of the magnetic flux density distribution of a uniform horizontal deflection magnetic field on the tube axis Z with the distance from the centre of this distribution to the phosphor screen.
The centre of the flux density distribution is defined as the position showing the maximum value Bp of the flux density distribution. The magnetic path length a is defined as the distance between the points where the density value is half the maximum value Bp, and A is defined as the distance from the centre Mc of the flux density distribution to the face plate. The spot S5a at the centre of the screen is shown in Figure 5a and comprises core Sc. As shown in Figure 5b, when spot S5b having flares Sf is formed at the screen periphery, the dimension of the horizontal direction of the flares is FH and the dimension of the vertical direction is FV. It was found that in this case the relationship shown in Figure 6 exists between a/A and FV/FH. Having ascertained that it is necessary that the value of FV/FH when evaluated from the practical point of view should be at least 0.5 and not more than 2.0, when this is substituted in Figure 6, the practical range of a is from 0.1 to 0.4. Preferably, the range of a/A is 0.2 to 0.3. The most ideal condition is obtained when a=0.2₅, when the flare Sf is circular and at its minimum size.
Figure 7 shows, respectively, the shapes S7a and S7b of the electron beam spot at the centre and at the periphery of the screen when a/A=0.2₅. To further improve the electron beam spot shape S7b in Figure 7 at the peripheral regions of the screen, the focal point distances of the electron lenses of the electron guns are adjusted at the peripheral regions of the screen. Spot S8b in Figure 8b shows an example of the improvement which this makes possible. As shown by S8a, the shape of the spot at the centre of the screen is unchanged.
The electron beam spot shape is further improved by the above construction. Convergence of the three electron beams over the entire surface of the face plate is further improved in the above construction of this invention by making the three electron beams generated from the electron guns substantially parallel and providing a time delay in the times with which the signals that are applied to the three electron guns are mutually controlled in a manner known per se.
The method by which this is done will now be described. When the various colour picture signals are input at the same time to the three electron guns, the electron beam spots on the face plate are separated from each other by a constant amount Δ. However, in this method, the time at which the signal is applied to the second electron gun is delayed by a time with respect to the time at which the signal is applied to the first electron gun, and the time at which the signal is applied to the third electron gun is delayed by a time _T with respect to the time at which the signal is applied to the second electron gun. If the horizontal width of the screen is H, the horizontal deflection frequency is fH, and the constant determined by the overscan is C, by making the-delay time _T=CA/fHH, electron beam spot convergence can be achieved over the whole area of the screen.
The amount of offset A of the spots of the three electron beams is one factor in this invention, so it is preferable to keep this A constant over the entire screen surface. To this end, the vertical deflection magnetic field must be made barrel-shaped.
The effect that the barrel-shaped magnetic field has on the offset amount A is given by:
In this equation, Hz is a coefficient indicating the non-uniformity of the magnetic field and is defined by
Y is the amount of deflection of the beam from the tube axis of the colour cathode ray tube, and increases with increased proximity to the face plate. Zs represents the distance from the face plate to the starting point of deflection. Thus, the effect of the barrel-shaped magnetic field on the amount of offset A is greater, the larger the value of Y, i.e. with increased proximity of the deflecting magnetic field to the face plate.
The extent of the flares is proportional to
In this formula (2), the effect of the term (Z-Zs) is augmented in comparison with formula (1). This shows that flares are generated uniformly comparatively irrespective of position in the magnetic field. Consequently, to keep the amount of offset A constant by a magnetic field with minimum non-uniformity, while suppressing the production of flares as far as possible, it is important to form the barrel-shaped magnetic field as near to the face plate as possible.
When applying this invention to large colour cathode ray tubes or tubes with a large angle of deflection, such as 110 degrees, the mutual positional relationship between the horizontal deflection magnetic field and the vertical deflection magnetic field should be optimised. By this means, the residual convergence error can be reduced over the entire surface of the screen than the centre of the vertical deflection magnetic field. Referring to Figure 2, a glass envelope 10 is provided with a face plate 11, a funnel 12 integrally sealed to this face plate 11, and a neck 14 is connected to the funnel.
The inside face of face plate 11 is formed with a phosphor screen 15 for picture display. This phosphor screen is made up of a regular arrangement of phosphor dots or phosphor stripes that emit red, green and blue light. A shadow mask 16 is arranged facing and adjacent to screen 15. Shadow mask 16 normally comprises a thin iron plate of dome shape matching the...Internal shape of face plate 11 and the portion facing screen 15 is formed with a large number of apertures 16, so arranged that three electron beams 20 impinge correctly on the phosphors of the corresponding colour.
Electron guns 17, which generate the three electron beams used for the three colours red, green and blue, are sealed into neck 14. The electron beams 20 are disposed in-line in the horizontal direction, i.e. the electron beams lie in the same horizontal plane. The arrangement is such that the electron beams are emitted substantially parallel to each other with a mutual separation of about 6.6 mm. The electron guns are integrated as a single unit comprising electron emitting cathodes and common electrodes of control, screen, focus and convergence cup electrodes. These are supplied with respective prescribed voltages. The potential of the high voltage electrodes as the convergence cup is usually ultra high potential (25 kV). The phosphor screen and shadow mask are maintained at an equivalent potential of 25kV as same as the high voltage electrode by a power source 21.
A deflection device 19 is mounted in the vicinity of the region (usually called the "cone" 13) where neck 14 joins funnel 12.
The picture signal is input between the cathodes and control electrodes corresponding to the respective electron beams. In scanning, if the "blue" beam is the leading beam, passing over the screen first, the blue picture signal is input first across the electrodes. The picture signals of the "green" and "red" beams, which follow the "blue" beam with a certain offset, are then input, as described above, with respective time delays τ and 2_T. These delays are produced by a delay element 18.
Deflection device 19 comprises a saddle- shaped horizontal deflection coil 22 that generates a uniform magnetic field H, as shown in Figure 3a, which constitutes the magnetic field that deflects electron beams 20 in the horizontal direction, and a toroidal vertical deflection coil 23 that generates a barrel-shaped magnetic field V, as shown in Figure 3b, which constitutes the field that deflects the beam in the vertical direction. The deflection coils are designed such that the half-width a of the flux density distribution on the tube axis of the horizontal deflection magnetic field and the vertical deflection magnetic field is 0.25 times the distance A from the centre of the flux density distribution to the phosphor screen. Deflection device 19 is driven by deflection driver J9₁.
For a 20 inch 90 degree deflection tube the horizontal width of the picture (phoshor screen) is about 400 mm. If it is assumed that the horizontal deflection frequency is 15.75 kHz, the amount of mutual offset 6 of the electron beam spots on the screen is 6.6 mm, and the constant C is 0.75, then the time delay of input of the picture signals for the various colours to the respective electron guns is about 0.8 microsecond.
The device produces pictures where the distortion of beam spot core and flare is minimised at both the centre and the corner of the screen so that the pictures are bright and with high resolution over the whole screen.
In another embodiment of this invention, 26 inch 110 degree deflection tubes were used, while the other conditions were the same as in the preceding embodiment. When an evaluation was made of such colour cathode ray tubes with a/A equal to 0.1 and a/A equal to 0.4, respectively, it was found that, in both cases, better performance was obtained than with a conventional system, in which the horizontal deflection magnetic field is of the pin cushion type. When a/A was set to 0.2 to 0.3, performance was even further improved.
Although in the 20 inch 90 degree deflection tube of the above embodiment the centres of the horizontal and vertical deflection magnetic fields were set at about 290 mm from the phosphor screen, in another embodiment of the invention, as shown in Figure 9, the position of the centre Hc of the horizontal deflection magnetic field is set at about 285 to 280 mm from the phosphor screen, and the position of the centre Vc of the vertical deflection magnetic field is set at about 295 to 300 mm from the phoshor screen.
In other words the centre Hc of the horizontal deflection magnetic field is advanced from the centre Vc of the vertical deflection magnetic field towards the phosphor screen 15 by an amount in the range 10 to 20 mm. It is found that this results in a further substantial improvement in the convergence accuracy attainable with three electron beams.
This invention has been described above under the assumption that, in the undeflected state, the electron beams are substantially parallel. This, of course, includes the case where they are geometrically parallel. However, without departing from the essence of this condition, the invention can, of course, also be applied to a colour cathode ray tube wherein colour offset correction is performed by applying constant delay times to the respective colour signals, although, under conditions of zero deflection, the three electron beams are actually out of convergence, i.e. are substantially non-coincident.
Usually a static convergence device is mounted on the electron gun side of the deflection coils and its hexapolar magnetic flux component leaks into the deflection magnetic field. To cancel this leakage component, the deflection field with hexapolar component compensation magnetic field as a result is, of course, also included in the uniform deflection magnetic field.

Claims

1. A colour cathode ray tube device comprising

an envelope (10) having a face plate (11), a funnel (12) and a neck (14);

a phosphor screen (15) formed on the inside of said face plate (11) and which emits light in the three colours, red, green and blue;

in-line electron guns (17) arranged in the neck to generate and direct three electron beams (20) towards the screen, the beams being in-line and mutually parallel in the horizontal direction of said phosphor screen (15);

a shadow mask (16) arranged in the vicinity of said phosphor screen (15) and having a large number of apertures to make said electron beams selectively impinge on said screen; and

a deflection device (19) attached outside said funnel and comprising a first magnetic field generating device (22) that generates a substantially uniform horizontal deflection magnetic field that deflects said electron beams (20) in the horizontal direction;

a second magnetic field generating device (23) that generates a barrel-shaped vertical deflection magnetic field that deflects said beams (20) in the vertical direction; and

means for applying a time delay to the time at which the picture signals of the respective colours red, green and blue input to said electron guns (17) are controlled; characterised in that

the half-width (a) on the tube axis, of the magnetic flux density distribution of said horizontal deflection magnetic field is in the range from 0.1 to 0.4 times the distance (A) from the centre of said flux density distribution to said phosphor screen (15).

2. The colour cathode ray tube device according to claim 1, characterised in that the half-width (a) of the magnetic flux density distribution of the tube device axis of said horizontal deflection magnetic field is within the range 0.2 to 0.3 times the distance (A) from the centre of said flux density distribution to said phosphor screen.

3. The colour cathode ray tube device according to claim 1 or 2, characterised in that the centre of the flux density distribution of the horizontal deflection magnetic field is arranged closer to said screen than is the centre of the flux density distribution of said vertical deflection magnetic field.